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Classical mechanics
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Work
Expressed in (SI unit): joule
Commonly used symbols: W
Expressed in other quantities: W = F · d

W = τ θ

In physics, mechanical work is the amount of energy transferred by a force acting through a distance. Like energy, it is a scalar quantity, with SI units of joules. The term work was first coined in 1826 by the French mathematician Gaspard-Gustave Coriolis.[1][2]

According to the work-energy theorem if an external force acts upon a rigid object, causing its kinetic energy to change from Ek1 to Ek2, then the mechanical work (W) is given by:[3]

W = \Delta E_k = E_{k_2} - E_{k_1} = \tfrac12 m (v_2^2 - v_1^2) \,\!

where m is the mass of the object and v is the object's velocity.

If the resultant force F on an object acts while the object is displaced a distance d, and the force and displacement act parallel to each other, the mechanical work done on the object is the product of F multiplied by d:[4]

W = F \cdot d

If the force and the displacement are parallel and in the same direction, the mechanical work is positive. If the force and the displacement are parallel but in opposite directions (i.e. antiparallel), the mechanical work is negative.

However, if the force and the displacement act perpendicular to each other, zero work is done by the force:[4]

W = 0\;

Contents

Units

The SI unit of work is the joule (J), which is defined as the work done by a force of one newton acting over a distance of one meter. This definition is based on Sadi Carnot's 1824 definition of work as "weight lifted through a height", which is based on the fact that early steam engines were principally used to lift buckets of water, through a gravitational height, out of flooded ore mines. The dimensionally equivalent newton-meter (N·m) is sometimes used instead; however, it is also sometimes reserved for torque to distinguish its units from work or energy.

Non-SI units of work include the erg, the foot-pound, the foot-poundal, and the liter-atmosphere.

Heat conduction is not considered to be a form of work, since the energy is transferred into atomic vibration rather than a macroscopic displacement

Zero work

A baseball pitcher does positive work on the ball by transferring energy into it.

Work can be zero even when there is a force. The centripetal force in a uniform circular motion, for example, does zero work since the kinetic energy of the moving object doesn't change. This is because the force is always perpendicular to the motion of the object; only the component of a force parallel to the velocity vector of an object can do work on that object. Likewise when a book sits on a table, the table does no work on the book despite exerting a force equivalent to mg upwards, because no energy is transferred into or out of the book.

Mathematical calculation

Force and displacement

Force and displacement are both vector quantities and they are combined using the dot product to evaluate the mechanical work, a scalar quantity:

W = \bold{F} \cdot \bold{d} = F d \cos\phi            (1)

where \textstyle\phi is the angle between the force and the displacement vector.

In order for this formula to be valid, the force and angle must remain constant. The object's path must always remain on a single, straight line, though it may change directions while moving along the line.

In situations where the force changes over time, or the path deviates from a straight line, equation (1) is not generally applicable although it is possible to divide the motion into small steps, such that the force and motion are well approximated as being constant for each step, and then to express the overall work as the sum over these steps.

The general definition of mechanical work is given by the following line integral:

W_C = \int_{C} \bold{F} \cdot \mathrm{d}\bold{s}             (2)

where:

\textstyle _C is the path or curve traversed by the object;
\bold F is the force vector; and
\bold s is the position vector.

The expression \delta W = \bold{F} \cdot \mathrm{d}\bold{s} is an inexact differential which means that the calculation of \textstyle{ W_C} is path-dependent and cannot be differentiated to give \bold{F} \cdot \mathrm{d}\bold{s}.

Equation (2) explains how a non-zero force can do zero work. The simplest case is where the force is always perpendicular to the direction of motion, making the integrand always zero. This is what happens during circular motion. However, even if the integrand sometimes takes nonzero values, it can still integrate to zero if it is sometimes negative and sometimes positive.

The possibility of a nonzero force doing zero work illustrates the difference between work and a related quantity, impulse, which is the integral of force over time. Impulse measures change in a body's momentum, a vector quantity sensitive to direction, whereas work considers only the magnitude of the velocity. For instance, as an object in uniform circular motion traverses half of a revolution, its centripetal force does no work, but it transfers a nonzero impulse.

Torque and rotation

Work done by a torque can be calculated in a similar manner. A torque \tau\; applied through a revolution of \theta\;, expressed in radians, does work as follows:

W= \tau \theta\

Mechanical energy

The mechanical energy of a body is that part of its total energy which is subject to change by mechanical work. It includes kinetic energy and potential energy. Some notable forms of energy that it does not include are thermal energy (which can be increased by frictional work, but not easily decreased) and rest energy (which is constant as long as the rest mass remains the same).

If an external force \textstyle\bold{F} acts upon a rigid body, causing its kinetic energy to change from \textstyle E_{k_1} to \textstyle E_{k_2}, then:[5]

\textstyle W = \Delta E_k = E_{k_2} - E_{k_1} = \frac{1}{2} mv_2 ^2 - \frac{1}{2} mv_1 ^2 = \frac{1}{2} m \Delta (v^2).

Thus we have derived the result, that the mechanical work done by an external force acting upon a rigid body is proportional to the difference in the squares of the speeds. Observe that the last term in the equation above is \textstyle\Delta (v^2) rather than \textstyle(\Delta v)^2.

The principle of conservation of mechanical energy states that, if a system is influenced by conservative forces (e.g. only to a gravitational force), and, or the sum of the work of all the other forces acting on the object is zero, its total mechanical energy remains constant throughout the process.

For instance, if an object with constant mass is in free fall, the total energy of position 1 will equal that of position 2.

(E_k + E_p)_1 = (E_k + E_p)_2 \,\!

where

The external work will usually be done by the friction force between the system on the motion or the internal non-conservative force in the system or loss of mechanical energy due to heat.

Frame of reference

The work done by a force acting on an object depends on the inertial frame of reference, because the distance covered while applying the force does. Due to Newton's law of reciprocal actions there is a reaction force; it does work depending on the inertial frame of reference in an opposite way. The total work done is independent of the inertial frame of reference.

References

  1. ^ Jammer, Max (1957). Concepts of Force. Dover Publications, Inc.. ISBN 0-486-40689-X. 
  2. ^ Sur une nouvelle dénomination et sur une nouvelle unité à introduire dans la dynamique, Académie des sciences, August 1826
  3. ^ Tipler (1991), page 138.
  4. ^ a b Resnick, Robert and Halliday, David (1966), Physics, Section 7-2 (Vol I and II, Combined edition), Wiley International Edition, Library of Congress Catalog Card No. 66-11527
  5. ^ Zitzewitz,Elliott, Haase, Harper, Herzog, Nelson, Nelson, Schuler, Zorn (2005). Physics: Principles and Problems. McGraw-Hill Glencoe, The McGraw-Hill Companies, Inc.. ISBN 0-07-845813-7. 

Bibliography

  • Serway, Raymond A.; Jewett, John W. (2004). Physics for Scientists and Engineers (6th ed. ed.). Brooks/Cole. ISBN 0-534-40842-7. 
  • Tipler, Paul (1991). Physics for Scientists and Engineers: Mechanics (3rd ed., extended version ed.). W. H. Freeman. ISBN 0-87901-432-6. 

External links


Simple English

In physics, work is the amount of energy transferred by a force.

Like energy, it is a scalar quantity, with SI units of joules. Heat conduction is not considered to be a form of work, since there is no macroscopically measurable force, only microscopic forces occurring in atomic collisions. The term work was created in the 1830s by the French mathematician Gaspard-Gustave Coriolis.[1]

According to the work-energy theorem if an external force acts upon a rigid object, causing its kinetic energy to change from Ek1 to Ek2, then the mechanical work (W) is given by:[2]

W = \Delta E_k = E_{k_2} - E_{k_1} = \frac{mv_2^2}{2} - \frac{mv_1^2}{2}

where m is the mass of the object and v is the object's velocity.

If a force F acts on an object while the object is displaced a distance d, and the force and displacement are parallel to each other, the work done on the object is the product of F and d:[3]

W = F \cdot d

If the force and the displacement are in the same direction, the work is positive. If the force and the displacement are in opposite directions the work is negative.

References

  1. Jammer, Max (1957). Concepts of Force. Dover Publications, Inc.. ISBN 0-486-40689-X. 
  2. Tipler (1991), page 138.
  3. Resnick, Robert and Halliday, David (1966), Physics, Section 7-2 (Vol I and II, Combined edition), Wiley International Edition, Library of Congress Catalog Card No. 66-11527

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